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Published byWendy Morris Modified over 6 years ago
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ILCDR08 10 July 2008 Plan of measuring cloud density in the solenoid field and in the quadrupole field K. Kanazawa (KEK)
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Contents Density measurement with solenoid field.
Density measurement in a quadrupole magnet Summary
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Density measurement with solenoid field (1)
The Point Given a solenoid field and the position of detection, the energy of measured electrons is automatically selected (=the volume is automatically defined). The detector in a chamber wall can catch high energy electrons produced near a beam. Vacuum chamber design Groove Monitor used without solenoid field Monitor used with solenoid field
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Density measurement with solenoid field (2)
Parameters Bunch size x = 0.434mm sy = 0.061mm sz = 6mm Number of positron in a bunch = 7.5x1010 (1.2mA) Solenoid field = 50 Gauss Simulation to check the idea (Fukuma) Orbits of kicked electrons near a bunch Orbits that reach the detector detector detector
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Density measurement with solenoid field (3)
Simulation by Fukuma Only these electrons reach the detector. Starting points of electrons that enter the detector Energy range +10 16 Y[mm] 8 E[keV] Beam 8 -10 -10 +10 X[mm] X[mm]
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Density measurement with solenoid field (4)
Inside of the chamber groove
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Density measurement with solenoid field (5)
Main Solenoid Compensation Solenoids Chamber with detectors
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Density measurement in a quadrupole magnet (1)
Electrons accelerated by a bunch along X-axis reach the detector. Electrons accelerated with small angle to X-axis moves spirally around X-axis losing their energy along X-axis to the spiral motion. Electrons with sufficient energy and direction close to X-axis reach the detector. With the help of simulation detector current is converted into the density near beam. X-axis Detector
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Density measurement in a quadrupole magnet (2)
Whole view Detector
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Summary By catching electrons interacted with a bunch, it will be possible to estimate the electron cloud density near the bunch in a magnetic field. The trial of measuring cloud density in the solenoid field and in the quadrupole field will be carried out this November at KEKB LER. Thank You!
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